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An Agnostic Sample Compression Scheme for Squared Loss of Near-Linear Size in the Fat-Shattering Dimension

Aug 2026 · 0 citations · 14 references
Computer Science

TL;DR

This scheme removes the dual factor entirely, including in the realizable case, from all previously known bounded-size constructions, agnostic and even realizable.

Abstract

We construct, for every function class $\mathcal{F}\subseteq[0,1]^{\mathcal{X}}$ and every accuracy $0<\alpha\le 1$, an agnostic sample compression scheme for the empirical squared loss: for every finite sample $S\in(\mathcal{X}\times[0,1])^m$ with arbitrary (noisy) labels, the scheme stores at most $O(\mathrm{fat}(\mathcal{F},c'\alpha)\cdot\log^3(2/\alpha))$ original labeled examples and auxiliary bits, independent of the sample size $m$, and reconstructs a function $\hat f$ with $L_2(\hat f,S)\le\inf_{f\in\mathcal{F}}L_2(f,S)+\alpha$. This resolves, in the positive, the open problem of Attias, Hanneke, Kontorovich, and Sadigurschi (ICML 2024, Section 5), which asks for an agnostic $\ell_2$ compression scheme of size $\mathrm{fat}(\mathcal{F},c\alpha)\cdot\mathrm{polylog}(c/\alpha)$. All previously known bounded-size constructions, agnostic and even realizable, incur a multiplicative dual fat-shattering factor, which can be exponentially larger than the primal dimension; our scheme removes the dual factor entirely, including in the realizable case. The dual factor in prior work enters solely through a sparsification step that forces uniform approximation on the sample. By targeting only a $(1-\epsilon)$-fraction of sample points, which suffices for an average-loss guarantee over a bounded range, K'egl's boosting margin bound yields $O(\log(1/\epsilon))$ rounds independent of $m$, and sparsification is never needed. The booster's synthetic target labels (values of a near-optimal $f^*\in\mathcal{F}$) are transmitted through quantized side-information bits attached to stored original examples, and the cross term of the squared loss forces the weak-learning scale $\Theta(\alpha)$, matching the same-scale form of the open problem.

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